ffdf478b62
all parameters as slip family-dependent
2023-08-04 13:07:42 -04:00
485839b651
consistent names
2023-08-01 18:03:00 +02:00
4191762a41
seems redundant
2023-08-01 11:07:07 +02:00
6b85ee47d4
new names
2023-08-01 10:49:43 +02:00
a113492600
example file updated
2023-07-28 11:21:27 +02:00
af2a4c6e72
more readable
2023-07-26 16:32:47 +02:00
2547d4a25c
clear names
2023-07-25 23:04:29 +02:00
c4134f2358
updated examples
2023-07-25 11:04:38 +02:00
9651f3e486
examples follow current implementation
...
small polishing/consistent capitalization
2023-07-17 18:03:31 +02:00
96de1abc04
forest projection of both edge and screw character with adjustment parameter f_edge
2023-06-22 14:16:27 -04:00
289765cae3
better values and documentation
2023-04-28 00:39:52 +02:00
eeb0825e63
adjusting to original publication
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Our implementation is using synonymous names for parameters compared to the paper by J.A. Wollmershauser, B. Clausen, and S.R. Agnew.
'xi_inf' and 'chi_inf' are not strictly "asymptotic values", but stresses that correspond to the back-extrapolation from the terminal linear hardening stage (characterized by 'h_inf_xi/chi').
All parameters are referenced back to their counterparts in the paper by J.A. Wollmershauser, B. Clausen, and S.R. Agnew.
2023-03-31 17:54:25 +00:00
13630325c3
notation following paper
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https://doi.org/10.1016/j.jmps.2016.10.012
DAMASK paper
2023-03-13 17:23:28 +01:00
e5b7ad335f
debug.yaml causes more work than it saves
2023-02-13 22:26:58 +01:00
f427b85967
re-fit for new phenopowerlaw formulation
2023-01-23 21:51:08 +01:00
1174e94486
re-fit
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- new phenopowerlaw formulation for hardening
- physics-based interactions (scaled DDD results such that
self-hardening is 1.0)
2023-01-15 01:34:30 +01:00
6c1edaeaac
new data for Aluminum
2023-01-15 01:33:50 +01:00
695d78eb35
have EOL and EOF
2023-01-08 14:32:13 +01:00
47e29f47fb
re-fit
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using higher order polynomial where appropriate. Code for fitting in
"parameters" repository
2023-01-08 14:31:54 +01:00
976cfd501a
thermal expansion coefficients for SiC
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this material was the initial motivation for adding fourth order
polynomials, but I could not find a reliable source for the graphs send
to damask@mpie.de . It seems that the CTE levels off for even higher
temperature which calls for a higher order polynomial
2023-01-08 14:31:43 +01:00
eb74d5a097
polishing
2023-01-08 11:54:42 +01:00
64fbfbb206
re-fit with correct conversion between Celsius and Kelvin
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procedure is documented in the 'parameters' repository
2023-01-08 10:58:01 +01:00
b9195a121f
commonly used scaling
2023-01-08 10:57:36 +01:00
1711bf3220
re-fit using correct scaling
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code is in 'parameters' repository
2023-01-08 10:57:06 +01:00
81870a6111
re-fit data
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some small adjustments, procedure is now reproducible using "parameters"
repository
2023-01-08 00:25:43 +01:00
8d9df30090
legacy example
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- undocumented
- not atomic
2023-01-07 22:01:03 +01:00
cca5d6d495
impoved naming
2022-12-09 06:48:16 +01:00
9d71ffa3ee
better naming
2022-11-24 11:23:10 +01:00
ef435ee7d1
commonly used variable name
2022-11-20 09:40:15 +01:00
28ea09050d
polishing
2022-10-25 23:18:22 +02:00
ff3e08531e
including test
2022-10-23 12:42:17 +02:00
0c83245d4b
example files for TWIP/TRIP
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I'm not able to reproduce the results from https://doi.org/10.1016/j.actamat.2016.07.032 ,
but these parameters give results that are qualitatively ok
2022-09-22 16:39:23 +02:00
576c79a619
following DAMASK paper
2022-06-13 14:08:45 +02:00
9b94aca09f
new example file
2022-06-08 23:28:54 +02:00
1b5194288b
polished tests, consistent variable name
2022-06-04 07:26:45 +02:00
77f586b1d7
Merge remote-tracking branch 'origin/development' into consistent-damage-parameter-names
2022-05-22 23:35:42 +02:00
0f1d0cbd61
copy and paste error
2022-05-17 08:53:32 +02:00
b3992e0ff0
test new example files
2022-05-16 23:24:29 +02:00
cda6e0af35
some difference to pure Ni
2022-05-13 11:44:02 +02:00
37eb567451
dataset for Platinum
2022-05-13 11:10:02 +02:00
8b3a0982c6
rename was missing (is already in code)
2022-04-27 05:58:05 +02:00
fb633798af
following paper
2022-04-01 19:47:40 +02:00
692b6d66ec
following hierarchical structure
2022-02-20 15:51:51 +01:00
909e1461b9
show thermal options
2022-02-19 23:11:10 +01:00
4cc7f94eef
guide the user
2022-02-19 23:10:05 +01:00
eca57d3b5f
Merge remote-tracking branch 'origin/development' into dislotwin-fix-TWIP-TRIP
2022-02-17 08:17:39 +01:00
bba105c2a8
re-fit, documented details
2022-02-13 18:37:34 +01:00
e3a64ae4ff
don't fit close to 0K
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cryogenic temperatures are normally not of interest, avoid considering
the strongly curved region below 80K in the fit gives probably better
extrapolation properties for T>300K
2022-02-13 14:57:01 +01:00
ba16ea21a0
avoid overfitting
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there are only 3 data points for C_13, with one close to 0K. Leave this
point out and fit only a 1st order polynomial
2022-02-13 14:48:15 +01:00
bb6a62c475
more temperature dependent data
2022-02-13 13:49:19 +01:00
Philip Eisenlohr